NSR Query Results
Output year order : Descending NSR database version of April 26, 2024. Search: Author = M.Plum Found 21 matches. 1992HO08 Phys.Rev. C46, 499 (1992) D.J.Horen, C.L.Morris, S.J.Seestrom, F.W.Hersman, J.R.Calarco, M.Holtrop, M.Leuschner, M.Rawool-Sullivan, R.W.Garnett, S.J.Greene, M.A.Plum, J.D.Zumbro Isospin Character of the Transition to the 0.803-MeV State in 206Pb from π± Scattering at 180 MeV NUCLEAR REACTIONS 206Pb(π+, π+), (π+, π+'), (π-, π-), (π-, π-'), E=180 MeV; measured missing mass spectra, σ(θ). 206Pb deduced neutron, proton matrix elements ratio for quadrupole, octupole transitions. Deformed optical model, DWIA analyses.
doi: 10.1103/PhysRevC.46.499
1992JO03 Phys.Rev. C46, 52 (1992) M.K.Jones, D.Dehnhard, S.K.Nanda, S.M.Sterbenz, C.L.Morris, M.Plum, J.D.Zumbro, A.H.Hussein, D.S.Oakley, M.J.Smithson, A.L.Williams, J.McDonald, M.A.Bryan, A.H.Fuentes, M.Lynker, D.Crockett, M.A.Machuca, S.Mordechai, C.F.Moore 4He(π, π'p)3H Reaction Near the P33 π-Nucleon Resonance NUCLEAR REACTIONS 4He(π+, π+'p), (π-, π-'p), E=140, 180 MeV; measured σ(θ(π'), σ(p)) vs excitation energy; deduced reaction mechanisms.
doi: 10.1103/PhysRevC.46.52
1991DO01 Phys.Rev. C43, 213 (1991) E.Donoghue, C.Glashausser, N.Hintz, A.Sethi, J.Shepard, R.Fergerson, M.Franey, M.Gazzaly, K.Jones, J.McClelland, S.Nanda, M.Plum Measurement of Spin Observables in the 28Si(p(pol), p(pol)') Reaction at 500 MeV and Comparison with the Distorted-Wave Impulse Approximation NUCLEAR REACTIONS 28Si(polarized p, p'), E=500 MeV; measured σ(Ep'), σ(θ), analyzing power vs θ, spin-transfer observables. Nonrelativistic, relativistic impulse approximation analysis, other data included.
doi: 10.1103/PhysRevC.43.213
1991OA01 Phys.Rev. C44, 2058 (1991) D.S.Oakley, R.J.Peterson, S.J.Seestrom, C.L.Morris, M.A.Plum, J.D.Zumbro, A.L.Williams, M.A.Bryan, J.W.McDonald, C.F.Moore Energy Dependence of Pion Inelastic Scattering from 208Pb NUCLEAR REACTIONS 208Pb(π+, π+), (π+, π+'), (π-, π-), (π-, π-'), E=120, 250 MeV; calculated σ(θ). 208Pb levels deduced proton, neutron matrix elements ratio. Different structure models.
doi: 10.1103/PhysRevC.44.2058
1990CL02 Phys.Rev. C41, 2246 (1990) B.L.Clausen, J.T.Brack, M.R.Braunstein, J.J.Kraushaar, R.A.Loveman, R.J.Peterson, R.A.Ristinen, R.A.Lindgren, M.A.Plum Analysis of Pion Scattering to Stretched States in 60Ni and Other Nuclei using Woods-Saxon Wave Functions NUCLEAR REACTIONS 60Ni(π+, π+'), (π-, π-'), E=162 MeV; measured σ(θ). 14C, 28Si, 54Fe, 60Ni deduced stretched state parameters. Other data input.
doi: 10.1103/PhysRevC.41.2246
1990DE26 Phys.Rev. C42, 1137 (1990) R.de Swiniarski, D.Beatty, E.Donoghue, R.W.Fergerson, M.Franey, M.Gazzaly, C.Glashausser, N.Hintz, K.W.Jones, J.B.McClelland, S.Nanda, M.Plum Comparison of Schrodinger and Dirac Coupled-Channels Analyses of the 28Si(p, p')28Si Reaction at 500 MeV NUCLEAR REACTIONS 28Si(polarized p, p), (polarized p, p'), E=500 MeV; measured σ(θ), analyzing power vs θ; deduced model parameters. Schrodinger, Dirac coupled-channels analyses.
doi: 10.1103/PhysRevC.42.1137
1990JO04 Phys.Rev. C42, R807 (1990) M.K.Jones, D.Dehnhard, S.K.Nanda, S.M.Sterbenz, C.L.Morris, M.Plum, J.D.Zumbro, A.Hussein, D.S.Oakley, M.J.Smithson, A.L.Williams, J.McDonald, M.A.Bryan, A.H.Fuentes, M.Lynker, D.Crockett, M.A.Machuca, S.Mordechai, C.F.Moore 4He(π, π'p)3H Reaction: Quasifree and resonance scattering NUCLEAR REACTIONS 4He(π+, π+'p), (π-, π-'p), E=180 MeV; measured σ(θ(π), θp); deduced σ(π+)/σ(π-). DWIA calculation.
doi: 10.1103/PhysRevC.42.R807
1990SE11 Phys.Rev. C42, 1929 (1990) P.A.Seidl, M.A.Bryan, M.Burlein, G.R.Burleson, K.S.Dhuga, H.T.Fortune, R.Gilman, S.J.Greene, M.A.Machuca, C.F.Moore, S.Mordechai, C.L.Morris, D.S.Oakley, M.A.Plum, G.Rai, M.J.Smithson, Z.F.Wang, D.L.Watson, J.D.Zumbro Pion Double Charge Exchange on T = 2 Nuclei in the Δ(3/2, 3/2) Resonance Region NUCLEAR REACTIONS 12C, 16O, 44Ca, 56Fe(π+, π-), E=100-300 MeV; measured σ(θ) vs E.
doi: 10.1103/PhysRevC.42.1929
1989PL05 Phys.Rev. C40, 1861 (1989) M.A.Plum, R.A.Lindgren, J.Dubach, R.S.Hicks, R.L.Huffman, B.Parker, G.A.Peterson, J.Alster, J.Lichtenstadt, M.A.Moinester, H.Baer 180° Electron Scattering from 14C NUCLEAR REACTIONS 14C(e, e'), E=82-269 MeV; measured σ(E(e'), θ); deduced 14C, 14B Coulomb energy difference. 14C levels deduced structure coefficients, form factors, IAS.
doi: 10.1103/PhysRevC.40.1861
1988MO01 Phys.Rev.Lett. 60, 408 (1988) S.Mordechai, N.Auerbach, G.R.Burleson, K.S.Dhuga, M.Dwyer, J.A.Faucett, H.T.Fortune, R.Gilman, S.J.Greene, C.Laymon, C.F.Moore, C.L.Morris, D.S.Oakley, M.A.Plum, S.J.Seestrom-Morris, P.A.Seidl, M.J.Smithson, Z.F.Wang, J.D.Zumbro Giant Dipole Resonances Built on Isobaric Analog States in Pion Double Charge Exchange NUCLEAR REACTIONS 56Fe, 80Se, 208Pb(π+, π-), E at 292 MeV/c; measured σ(E(π-), θ(π-)), σ(θ(π-)). 56Ni, 80Kr, 208Po deduced giant dipole resonance parameters. Coupled-channel impulse approximation calculations.
doi: 10.1103/PhysRevLett.60.408
1987FA05 Phys.Rev. C35, 1570 (1987) J.A.Faucett, M.W.Rawool, K.S.Dhuga, J.D.Zumbro, R.Gilman, H.T.Fortune, C.L.Morris, M.A.Plum Pion Double Charge Exchange on 12C at Low Energies NUCLEAR REACTIONS 12C(π+, π-), E=50-120 MeV; measured σ(θ), σ(θ) vs E, σ(E(π-)); deduced σ energy dependence.
doi: 10.1103/PhysRevC.35.1570
1987HI09 Phys.Rev. C36, 485 (1987) R.S.Hicks, R.L.Huffman, R.A.Lindgren, G.A.Peterson, M.A.Plum, J.Button-Shafer Electroexcitation of Discrete Levels in 12C and High Momentum Transfers NUCLEAR REACTIONS 12,13C(e, e'), E=80-485 MeV; measured σ(E(e'), θ). 13,12C levels deduced transverse excitation form factors. Enriched 13C target. Shell model.
doi: 10.1103/PhysRevC.36.485
1987HU01 Phys.Rev. C35, 1 (1987) R.L.Huffman, J.Dubach, R.S.Hicks, M.A.Plum Phenomenological Wave Functions for the Ground and 2.313 MeV States in 14N NUCLEAR REACTIONS 14N(e, e), (e, e'), E=80-372.6 MeV; measured σ(E, θ). 14N level deduced form factors, wave functions; 14N(p, p'), (γ, π+), 14C(p, n), E=25-200 MeV; calculated σ(θ). 14N level deduced spectroscopic factors. Solid boron nitride, natural N2 gas targets. DWBA analysis.
doi: 10.1103/PhysRevC.35.1
1987LI30 Can.J.Phys. 65, 666 (1987) R.A.Lindgren, M.Leuschner, B.L.Clausen, R.J.Peterson, M.A.Plum, F.Petrovich Isovector Excitation of 1(h-bar x Omega) Stretched States in Nuclei: Effects of meson exchange currents, unbound wave functions, and knockout exchange amplitudes on the extraction of particle-hole strengths NUCLEAR REACTIONS 14C, 26Mg, 28Si, 54Fe, 60Ni(e, e'), E ≈ 136-205 MeV; analyzed σ(E(e'), θ(e')). 14C, 26Mg, 28Si, 54Fe, 60Ni deduced form factors, particle-hole strengths, amplitudes, B(λ). Meson exchange currents.
doi: 10.1139/p87-095
1987PE03 Phys.Rev. C35, 495 (1987) R.J.Peterson, B.L.Clausen, J.J.Kraushaar, R.A.Lindgren, M.A.Plum, W.W.Jacobs, H.Nann Proton Stripping to 8- Stretched States in 60Ni NUCLEAR REACTIONS 59Co(α, t), E=80.9 MeV; measured σ(θ). 60Ni deduced levels, J, π, T, spectroscopic factors. Magnetic spectrometer. DWBA analyses.
doi: 10.1103/PhysRevC.35.495
1986HI06 Phys.Rev. C34, 1161 (1986) R.S.Hicks, R.A.Lindgren, M.A.Plum, G.A.Peterson, H.Crannell, D.I.Sober, H.A.Thiessen, D.J.Millener M4 Excitations in 13C NUCLEAR REACTIONS 13C(e, e'), E=78-338 MeV; measured σ(E, θ). 13C levels deduced from factors, isoscalar, isovector transition amplitudes. Shell model.
doi: 10.1103/PhysRevC.34.1161
1986PA20 Phys.Rev. C34, 2354 (1986) B.Parker, R.S.Hicks, A.Hotta, R.L.Huffman, G.A.Peterson, M.A.Plum, P.J.Ryan, R.P.Singhal Transverse Quasielastic Electron Scattering from the Deuteron NUCLEAR REACTIONS 2H(e, e'), E=220, 270, 320 MeV; measured σ(E(e'), θ); deduced isobar configuration role.
doi: 10.1103/PhysRevC.34.2354
1986PE01 Phys.Rev. C33, 31 (1986) R.J.Peterson, B.L.Clausen, J.J.Kraushaar, H.Nann, W.W.Jacobs, R.A.Lindgren, M.A.Plum Proton Stripping to 6- Stretched States of 26Al NUCLEAR REACTIONS 24,25Mg(α, t), E=80.9 MeV; measured σ(Et), σ(θ). 26Al deduced levels, J, π, T, spectroscopic factors, stretched transition characteristics.
doi: 10.1103/PhysRevC.33.31
1984HU07 Phys.Lett. 139B, 249 (1984) R.L.Huffman, R.S.Hicks, J.Dubach, B.Parker, M.A.Plum, G.Lahm, R.Neuhausen, J.C.Bergstrom Comparison of Isoscalar and Isovector (e, e') M1 Form Factors at High Momentum Transfer NUCLEAR REACTIONS 14N(e, e), (e, e'), E not given; measured M1 form factors. 14N deduced isoscalar, isovector transition differences. Shell model comparison.
doi: 10.1016/0370-2693(84)91073-6
1984PL02 Phys.Lett. 137B, 15 (1984) M.A.Plum, R.A.Lindgren, J.Dubach, R.S.Hicks, R.L.Huffman, B.Parker, G.A.Peterson, J.Alster, J.Lichtenstadt, M.A.Moinester, H.Baer Isoscalar and Isovector M4 Spin Transitions in 14C NUCLEAR REACTIONS 14C(e, e'), E=100-300 MeV; measured σ(E(e')), transverse form factor. 14C levels deduced M4 spin transition density isoscalar, isovector amplitudes, σ(π+)/σ(π-). Pion data input.
doi: 10.1016/0370-2693(84)91096-7
1981LI19 Phys.Rev.Lett. 47, 1266 (1981) R.A.Lindgren, M.A.Plum, W.J.Gerace, R.S.Hicks, B.Parker, G.A.Peterson, R.Singhal, C.F.Williamson, X.K.Maruyama, F.Petrovich Isospin Splitting of Isovector High-Spin ' Stretched ' Particle-Hole Excitations in Non-Self-Conjugate Nuclei NUCLEAR REACTIONS 60Ni(e, e'), E=205 MeV; measured σ(θ(e), E(e)). 60Ni deduced levels, J, π, T, B(M8), isospin splitting. Lane model parametrization, stretched particle-hole excitations. NUCLEAR STRUCTURE 13C, 15N, 54,56Fe, 58,60Ni; calculated isospin splitting. Lane model parametrization, stretched particle-hole excitation.
doi: 10.1103/PhysRevLett.47.1266
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